Solution

ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2010/iii/paper-68/1/b/ii/solution

At , the phase is , so the ordinary nonstationary endpoint formula fails. In the degenerate endpoint in Laplace's method, take and extend the localized integral to infinity:
The last equality follows by . It is the value of the cubic Laplace transition integral after its normalization is rescaled to the coefficient .

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